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By the end of this section, you will be able to:
  • Explain how energy can be stored in a magnetic field
  • Derive the equation for energy stored in a coaxial cable given the magnetic energy density

The energy of a capacitor is stored in the electric field between its plates. Similarly, an inductor has the capability to store energy, but in its magnetic field. This energy can be found by integrating the magnetic energy density    ,

u m = B 2 2 μ 0

over the appropriate volume. To understand where this formula comes from, let’s consider the long, cylindrical solenoid of the previous section. Again using the infinite solenoid approximation, we can assume that the magnetic field is essentially constant and given by B = μ 0 n I everywhere inside the solenoid. Thus, the energy stored in a solenoid or the magnetic energy density times volume is equivalent to

U = u m ( V ) = ( μ 0 n I ) 2 2 μ 0 ( A l ) = 1 2 ( μ 0 n 2 A l ) I 2 .

With the substitution of [link] , this becomes

U = 1 2 L I 2 .

Although derived for a special case, this equation gives the energy stored in the magnetic field of any inductor. We can see this by considering an arbitrary inductor through which a changing current is passing. At any instant, the magnitude of the induced emf is ε = L d i / d t , so the power absorbed by the inductor is

P = ε i = L d i d t i .

The total energy stored in the magnetic field when the current increases from 0 to I in a time interval from 0 to t can be determined by integrating this expression:

U = 0 t P d t = 0 t L d i d t i d t = L 0 l i d i = 1 2 L I 2 .

Self-inductance of a coaxial cable

[link] shows two long, concentric cylindrical shells of radii R 1 and R 2 . As discussed in Capacitance on capacitance, this configuration is a simplified representation of a coaxial cable . The capacitance per unit length of the cable has already been calculated. Now (a) determine the magnetic energy stored per unit length of the coaxial cable and (b) use this result to find the self-inductance per unit length of the cable.

Figure a shows two concentrically arranged hollow cylinders. The radius of the inner one is R1 and that of the outer one is R2. Figure 2 shows a dotted circle with radius r in between the two cylinders. Figure c shows a cylinder of length and radius r in between the two cylinders. Its thickness is dr.
(a) A coaxial cable is represented here by two hollow, concentric cylindrical conductors along which electric current flows in opposite directions. (b) The magnetic field between the conductors can be found by applying Ampère’s law to the dashed path. (c) The cylindrical shell is used to find the magnetic energy stored in a length l of the cable.

Strategy

The magnetic field both inside and outside the coaxial cable is determined by Ampère’s law. Based on this magnetic field, we can use [link] to calculate the energy density of the magnetic field. The magnetic energy is calculated by an integral of the magnetic energy density times the differential volume over the cylindrical shell. After the integration is carried out, we have a closed-form solution for part (a). The self-inductance per unit length is determined based on this result and [link] .

Solution

  1. We determine the magnetic field between the conductors by applying Ampère’s law to the dashed circular path shown in [link] (b). Because of the cylindrical symmetry, B is constant along the path, and
    B · d l = B ( 2 π r ) = μ 0 I .

    This gives us
    B = μ 0 I 2 π r .

    In the region outside the cable, a similar application of Ampère’s law shows that B = 0 , since no net current crosses the area bounded by a circular path where r > R 2 . This argument also holds when r < R 1 ; that is, in the region within the inner cylinder. All the magnetic energy of the cable is therefore stored between the two conductors. Since the energy density of the magnetic field is
    u m = B 2 2 μ 0 = μ 0 I 2 8 π 2 r 2 ,

    the energy stored in a cylindrical shell of inner radius r , outer radius r + d r , and length l (see part (c) of the figure) is
    u m = B 2 2 μ 0 = μ 0 I 2 8 π 2 r 2 .

    Thus, the total energy of the magnetic field in a length l of the cable is
    U = R 1 R 2 d U = R 1 R 2 μ 0 I 2 8 π 2 r 2 ( 2 π r l ) d r = μ 0 I 2 l 4 π ln R 2 R 1 ,

    and the energy per unit length is ( μ 0 I 2 / 4 π ) ln ( R 2 / R 1 ) .
  2. From [link] ,
    U = 1 2 L I 2 ,

    where L is the self-inductance of a length l of the coaxial cable. Equating the previous two equations, we find that the self-inductance per unit length of the cable is
    L l = μ 0 2 π ln R 2 R 1 .

Significance

The inductance per unit length depends only on the inner and outer radii as seen in the result. To increase the inductance, we could either increase the outer radius ( R 2 ) or decrease the inner radius ( R 1 ) . In the limit as the two radii become equal, the inductance goes to zero. In this limit, there is no coaxial cable. Also, the magnetic energy per unit length from part (a) is proportional to the square of the current.

Check Your Understanding How much energy is stored in the inductor of [link] after the current reaches its maximum value?

0.50 J

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Summary

  • The energy stored in an inductor U is
    U = 1 2 L I 2 .
  • The self-inductance per unit length of coaxial cable is
    L l = μ 0 2 π ln R 2 R 1 .

Conceptual questions

Show that L I 2 / 2 has units of energy.

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Problems

At the instant a current of 0.20 A is flowing through a coil of wire, the energy stored in its magnetic field is 6.0 × 10 −3 J . What is the self-inductance of the coil?

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Suppose that a rectangular toroid has 2000 windings and a self-inductance of 0.040 H. If h = 0.10 m , what is the current flowing through a rectangular toroid when the energy in its magnetic field is 2.0 × 10 −6 J ?

0.01 A

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Solenoid A is tightly wound while solenoid B has windings that are evenly spaced with a gap equal to the diameter of the wire. The solenoids are otherwise identical. Determine the ratio of the energies stored per unit length of these solenoids when the same current flows through each.

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A 10-H inductor carries a current of 20 A. How much ice at 0 ° C could be melted by the energy stored in the magnetic field of the inductor? ( Hint : Use the value L f = 334 J/g for ice.)

6.0 g

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A coil with a self-inductance of 3.0 H and a resistance of 100 Ω carries a steady current of 2.0 A. (a) What is the energy stored in the magnetic field of the coil? (b) What is the energy per second dissipated in the resistance of the coil?

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A current of 1.2 A is flowing in a coaxial cable whose outer radius is five times its inner radius. What is the magnetic field energy stored in a 3.0-m length of the cable?

U m = 7.0 × 10 −7 J

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Questions & Answers

Is it possible to find the magnetic field of a circular loop at the centre by using ampere's law?
Rb Reply
Is it possible to find the magnetic field of a circular loop at it's centre?
Rb Reply
yes
Brother
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A hot liquid at 80degree Celsius is added to 600g of the same liquid originally at 10 degree Celsius. when the mixture reaches 30 degree Celsius, what will be the total mass of the liquid?
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what is electrostatics
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Study of charges which are at rest
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Explain Kinematics
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Using the same two positive charges, the left positive charge is increased so that its charge is 4 times LARGER than the charge on the right. Using your notes on Coulomb's law and changes to the charge, once the charge is increased, what is the new force of repulsion between the two positive charges?
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A closely wound search coil has an area of 4cm^2,1000 turns and a resistance of 40ohm. It is connected to a ballistic galvanometer whose resistance is 24 ohm. When coil is rotated from a position parallel to uniform magnetic field to one perpendicular to field,the galvanometer indicates a charge
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Using Kirchhoff's rules, when choosing your loops, can you choose a loop that doesn't have a voltage?
Michael Reply
how was the check your understand 12.7 solved?
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Who is ISSAAC NEWTON
LOAK Reply
he's the father of 3 newton law
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he is Chris Issaac's father :)
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Practice Key Terms 1

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Source:  OpenStax, University physics volume 2. OpenStax CNX. Oct 06, 2016 Download for free at http://cnx.org/content/col12074/1.3
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